How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Burgers centered rarefaction and trace
Example
Assume the Axiom of Countable Choice. Let , let with , and set . For define Let for and for , with any value at . Then is continuous for , satisfies the initial-value weak identity for , and satisfies with equality the initial entropy identity for every convex with compatible flux and every Kružkov pair , , where . For every compact interval and , so strongly in as .
Example references
Facts & Assumptions
Given: Countable Choice; the states ; the Burgers flux, fan, initial data, and entropy pairs in the Example.
Strictly convex scalar Riemann construction: for with on , the inverse-characteristic fan in the Statement satisfies the initial-value weak identity, compatible convex entropy inequalities, and Kružkov inequalities.
Riemann shock and rarefaction waves for are weak solutions, and the shock is an entropy solution: assuming Countable Choice, the Burgers fan is a weak solution and satisfies every declared convex and Kružkov entropy inequality, with equality.
The Axiom of Countable Choice (): Countable Choice is the choice assumption used by the imported Lebesgue weak formulation.
Distributional systems and entropy flux pairs: for smooth tests compactly supported in , the scalar initial weak identity is ; the entropy inequality replaces by , requires a nonnegative test, and requires the whole integral to be nonnegative.
.
Proof
The Burgers flux satisfies and on . Thus [F1] applies, and its inverse profile is for , with the two constant branches displayed in the Example. It gives the weak and entropy identities with the specified initial trace in the formulation of [F4]; [F2] independently confirms the same Lebesgue formulation under [F3].
In the fan, and , so ; the constant branches solve the equation, and the traces match at and . The fan values stay in . The profile and initial step agree outside , whose length is at most , and their values differ by at most . This proves the stated local estimate, including when both characteristic speeds have the same sign.